Girkmann problem with a Discrete Element Method
DOI: https://doi.org/10.20528/cjsmec.2016.08.017
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Cells of Voronoï are used as particles in the Discrete Element code CeaMka3D. This type of meshing does not leave geometrical space like that can be the case with spherical particles. This method has already been used successfully to simulate the propagation of seismic waves in a linear elastic medium in 2D or in 3D. In this paper, a specific axisymmetric formulation is presented. In a first part, the calculation of the volumetric deformation of a particle and the forces between particles are described. In a second part, the specific forces for the axisymmetric formulation are described. At last, this formulation is tested for the Girkmann problem. This axisymmetric benchmark has been presented in January 2008 by the International Association of Computational Mechanics (IACM) in order to test the singularity at the junction between shell and beam. The accuracy of the axisymmetric formulation for this Discrete Element Method is evaluated by this benchmark. The results of this Discrete Element Method are compared with others numerical methods.
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Cundall PA, Strack ODL (1979). A discrete numerical model for granular assemblies. Geotechnique, 29(1), 47-65.
http://dx.doi.org/10.1680/geot.1979.29.1.47
Devloo PRB, Farias AM, Gomes SM, Gonçalves JL (2013). Application of a combined continuous-discontinuous Galerkin finite element method for the solution of the Girkmann problem. Computers and Mathematics with Applications, 65, 1786-1794.
http://dx.doi.org/10.1016/j.camwa.2013.03.015
Girkmann K (1956). Flächentragwerke. 4th ed. Springer-Verlag, Wien.
http://dx.doi.org/10.1007/978-3-7091-4386-5
Hoover WG, Arhurst WT, Olness RJ (1974). Two-dimensional studies of crystal stability and fluid viscosity. Journal of Chemical Physics, 60, 4043-4047.
http://dx.doi.org/10.1063/1.1680855
Mariotti C (2007). Lamb's problem with the lattice model Mka3D. Geophysical Journal International, 171, 857-864.
http://dx.doi.org/10.1111/j.1365-246X.2007.03579.x
Mariotti C (2015). A new Leapfrog scheme for rotational motion in 3D. International Journal for Numerical Methods in Engineering, 107, 273-289.
http://dx.doi.org/10.1002/nme.5165
Mariotti C, Monasse L (2012). From General Mechanics to Discontinuity, Unified Approach to Elasticity. Presses des Ponts, France.
Mariotti C, Le Piver F, Aubry L (2015). A least-squares coupling method between a finite element code and a discrete element code. International Journal for Numerical Methods in Engineering, 101(10), 731-743.
http://dx.doi.org/10.1002/nme.4822
Monasse L, Mariotti C (2012). An energy-preserving Discrete Element Method for elastodynamics. ESAIM: Mathematical Modelling and Numerical Analysis, 46(6), 1527-1553.
http://dx.doi.org/10.1051/m2an/2012015
Pitkäranta J, Babuska I, Szabo B (2008). The Girkmann problem. IACM Expression, January 2008, 22-28.
Szabo B, Babuska I, Pitkäranta J, Nervi S (2010). The problem of verification with reference to the Girkmann problem. Engineering with Computers, 26, 171-183.
http://dx.doi.org/10.1007/s00366-009-0155-0
Timoshenko SP, Woinowsky-Krieger S (1959). Theory of Plates and Shells. McGraw-Hill, New York.








